scholarly journals Effect of the doubly magic shell closures in Sn132 and Pb208 on the mass distributions of fission fragments of superheavy nuclei

2020 ◽  
Vol 101 (1) ◽  
Author(s):  
C. Ishizuka ◽  
X. Zhang ◽  
M. D. Usang ◽  
F. A. Ivanyuk ◽  
S. Chiba
2019 ◽  
Vol 49 (12) ◽  
pp. 122001
Author(s):  
DONG GuoXiang ◽  
CHEN YongJing ◽  
WANG XiaoBao ◽  
WANG HuaLei ◽  
HAO YiWei ◽  
...  

2020 ◽  
Vol 51 (1) ◽  
pp. 136-143
Author(s):  
S. Subramanian ◽  
M. T. Senthil Kannan ◽  
S. Selvaraj

Author(s):  
E. V. PROKHOROVA ◽  
M. G. ITKIS ◽  
YU. TS. OGANESSIAN ◽  
E. M. KOZULIN ◽  
A. A. BOGATCHEV ◽  
...  

2003 ◽  
Vol 20 (10) ◽  
pp. 1702-1705 ◽  
Author(s):  
Wu Zhe-Ying ◽  
Xu Fu-Rong ◽  
Zhao En-Guang ◽  
Zheng Chun-Kai

2016 ◽  
Vol 761 ◽  
pp. 125-130 ◽  
Author(s):  
R. Léguillon ◽  
K. Nishio ◽  
K. Hirose ◽  
H. Makii ◽  
I. Nishinaka ◽  
...  

Author(s):  
Gayatri Sarkar ◽  
Moumita Maiti ◽  
Amandeep Kaur ◽  
Manoj K. Sharma

The decay dynamics of 197Tl* compound nucleus has been studied within the framework of the dynamical cluster-decay model (DCM) at above barrier energy Ec.m. ≈ 100 MeV using quadrupole deformed configuration of decay fragments. The influence of various nuclear radius parameters on the decay path and mass distributions has been investigated by analysing the fragmentation potential and preformation probability. It is observed that 197Tl* nucleus exhibits the triple-humped mass distribution, independent of nuclear radius choice. The most preferred fission fragments of both fission modes (symmetric and asymmetric) are identified, which lie in the neighborhood of spherical and deformed magic shell closures. Moreover, the modification in the barrier characteristics, such as interaction barrier and interaction radius, is observed with the variation in the radius parameter of decaying fragments and influences the penetrability and fission cross-sections. Finally, the fission cross-sections are calculated for considered choices of nuclear radii, and the results are compared with the available experimental data.


2018 ◽  
Vol 27 (05) ◽  
pp. 1850043 ◽  
Author(s):  
Amandeep Kaur ◽  
Gudveen Sawhney ◽  
Manoj K. Sharma ◽  
Raj K. Gupta

The temperature-dependent preformed cluster model [PCM[Formula: see text]] is employed to extend our recent work [Niyti, G. Sawhney, M. K. Sharma and R. K. Gupta, Phys. Rev. C 91 (2015) 054606] on [Formula: see text]-decay chains of various isotopes of [Formula: see text]–118 superheavy nuclei (SHN), to spontaneous fissioning nuclei [Formula: see text]Lr, [Formula: see text]Rf, [Formula: see text]Db, [Formula: see text]Rg, and [Formula: see text]Cn occurring as end products of these [Formula: see text]-decay chains. The behavior of fragment mass distribution and competitive emergence of the dominant decay mode, i.e., the [Formula: see text]-emission versus spontaneous fission (SF), are studied for identifying the most probable heavy fission fragments, along with the estimation of SF half-life times T[Formula: see text] and total kinetic energy (TKE) of the above noted isotopes of [Formula: see text]–112 nuclei decaying via the SF process. The mass distributions of chosen nuclei are clearly symmetric, independent of mass and temperature. The most preferred decay fragment is found to lie in the neighborhood of doubly magic shell closures of [Formula: see text] and [Formula: see text], with largest preformation factor [Formula: see text]. In addition, a comparative study of the “hot compact” and “cold elongated” configurations of [Formula: see text]-deformed and [Formula: see text]-oriented nuclei indicates significantly different behaviors of the two mass fragmentation yields, favoring “hot compact” configuration.


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